Even though the operatorsum representation gives an
internal view of the dynamics of an open system, we can still learn something
about the environment from the Ak operators. For a given evolution
map E and an input state _, define Wkl by
Show that these numbers are the matrix elements of the final
density operator of the environment E, if the initial state of E is pure (as in
Eq. 9.1).
To make this more definite, suppose the Kraus operators for
a qubit system are a1 and bZ, where a and b are real parameters such that a2
+ b2 = 1. First, confirm that this pair of operators is
»
Even though the operatorsum representation gives an
internal view of the dynamics of an open system, we can still learn something
about the environment from the Ak operators. For a given evolution
map E and an input state _, define Wkl by
Show that these numbers are the matrix elements of the final
density operator of the environment E, if the initial state of E is pure (as in
Eq. 9.1).
To make this more definite, suppose the Kraus operators for
a qubit system are a1 and bZ, where a and b are real parameters such that a2
+ b2 = 1. First, confirm that this pair of operators is
normalized according to Eq. 9.12. Then find the eigenvalues of the final
environment state when the input qubit states are
»
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